Optical modulating device

ABSTRACT

An optical modulation apparatus is provided which implements a stable amplifying function by reducing the effect of reflected light rays form end faces of a bidirectional optical amplifier by imposing a numerical limitation on the relationship between the gain of the bidirectional optical amplifier and the loss of the optical modulator, or by inserting a polarization rotation section in a reflection type optical modulator including the bidirectional optical amplifier or in a multi-wavelength collective optical modulation system combining the multiple optical modulators. An optical modulation apparatus is provided which implements a stable amplifying function and cost reduction by reducing the effect of reflected light rays by interposing optical isolators at every alternate SOAs in a transmission-type optical modulation apparatus including a plurality of semiconductor optical amplifiers (SOAs) connected in a multistage fashion.

TECHNICAL FIELD

The present invention relates to an optical modulation apparatus usedfor optical communication, and particularly to a constructing techniqueof the optical modulation apparatus constructed by combining an opticalamplifier such as a semiconductor optical amplifier with an opticalintensity modulator.

BACKGROUND ART

Conventionally, systems have been studied which apply multi-wavelengthlight including a plurality of optical carriers generated by an opticalshort-pulse laser or by amplitude modulation/phase modulation towavelength division multiplexing (WDM) signal transmission. Suchmulti-wavelength light has the same spectral spacing between individualside modes so that the channels obtained by wavelength demultiplexing ofthe side modes have the same wavelength spacing. Accordingly, suchmulti-wavelength light is simpler in wavelength constellation thanmulti-wavelength light based on a method of preparing separate lasersfor individual channels and setting wavelengths for the individualchannels.

To implement a WDM signal transmission system using the multi-wavelengthlight, one of the important problems is the simplification of theconfiguration of an optical modulation circuit and its economization.FIG. 1 shows a configuration of a conventional optical modulationcircuit. The multi-wavelength light generated by a multi-wavelengthlight source 101 undergoes wavelength demultiplexing by a wavelengthdemultiplexer 103, modulatinig by individual optical intensitymodulators 105, and multiplexing by a wavelength multiplexer 107 again.The configuration as shown in FIG. 1 requires two wavelengthmulti-demultiplexers 103 and 107 having the same absolute value in thetransmission central wavelengths. Thus, an optical modulation apparatuswith a configuration as shown in FIG. 2 is proposed which includes awavelength multi-demultiplexer 207, one or more optical intensitymodulators 209, and reflecting mirrors 211 equal to the opticalintensity modulators in the number (see, Japanese patent applicationLaid-open No. 2002-318374).

In the optical modulation apparatus as shown in FIG. 2, themulti-wavelength light, which is input to an input port 203 of anoptical input section 201, passes through an input/output port 205, andundergoes wavelength demultiplexing by a wavelength demultiplexer 207,modulating by individual optical intensity modulators 209, andreflection by optical reflectors 211. Then, the reflected light raysreturn the paths they have came with being multiplexed again by thewavelength multiplexer 207 and output from an output port 213 of theinput/output means 201. According to the system configuration, itincludes only one wavelength multi-demultiplexer 207. Consequently, itcan facilitate the matching of the transmission central wavelengths ofthe wavelength multi-demultiplexer, and reduce the cost of the system.

In either FIG. 1 or FIG. 2, the individual wavelengths have theiroptical power reduced by the losses of optical devices used by thewavelength multi-denultiplexer and the like. In addition, as for thesystem having the multi-wavelength light source and the opticalmodulators placed at a distance physically, the losses of fibertransmission paths linking them become nonnegligible. Since thereduction in the WDM signal power deteriorates the signal-to-noise ratio(SNR), the power must be amplified using an optical amplifier designatedby the reference numeral 109 of FIG. 1 or by 215 of FIG. 2.

FIGS. 1 and 2 each show an example which amplifies the WDM signal powerat once with a broadband optical amplifier that covers the entirewavelength band of the multi-wavelength light (see, Japanese patentapplication laid-open No. 2003-18853). The example employs apolarization independent optical amplifier that amplifies the opticalintensity without depending on the polarization of the modulated lightpassing through the wavelength division multiplexing. Such an opticalamplifier generally employs a fiber amplifier such as an erbium (Er)doped fiber amplifier (EDFA). The EDFA is an optical amplifier thatamplifies the light traveling through the fiber by doping the core ofthe silica glass fiber with erbium ions Er³⁺, and by utilizing thestimulated emission in the transition proper to the ions. On the otherhand, as an optical amplifier used for the optical communication, asemiconductor optical amplifier (SOA) has been developed. The SOA is anoptical amplifier that amplifies the light traveling through the activelayer of the semiconductor by the stimulated emission by reducing thereflectance of end faces of the cavity of the semiconductor laser.

Although both types of the optical amplifiers have a broad gainbandwidth of 30 nm or more, they differ greatly in the lifetime ofcarriers in the excited level. Since the EDFA has the gain broadeningestablished by the transition from a plurality of discrete excitationenergy levels, it has a long carrier lifetime of an order ofmilliseconds, and uneven gain broadening. In contrast with this, the SOAhas a short carrier lifetime of an order of nanoseconds, and the gainbroadening can be considered as uniform. Generally, the opticalamplifier operates in the saturation region of the gain to obtain largeoutput. When the optical amplifier with the uniform gain broadeningamplifies a plurality of different signal wavelengths in the saturationregion of the gain, the individual wavelengths scramble for the gain,which causes crosstalk between the channels and degrades the signalwaveform. Accordingly, fiber amplifiers such as the EDFA are usuallyused to amplify the WDM signal collectively as described above. However,comparing the SOA that excites the semiconductor by injection currentwith the EDFA that includes a semiconductor laser for outputting pumpinglight, a doped fiber doped with erbium or the like, and a coupler forcoupling the pumping light to the doped fiber, the SOA is far economicalfran the viewpoint of the number of components. In particular, the SOAis more suitable for amplifying a single signal wavelength.

To amplify the WDM signal collectively using the fiber amplifier, it isessential to increase the power of the optical amplifier to compensatefor the optical losses caused by optical components such as thewavelength multi-demultiplexer and optical intensity modulators.However, a broadband, high-power light amplifier covering the entirewavelength band of the multi-wavelength light is very expensive even ifused alone. Accordingly, depending on the wavelength bandwidth andoutput required, a configuration that amplifies the wavelengthsindividually by the SOAs can sometimes implement the optical modulationcircuit more cheaply than the configuration using the fiber amplifier.

In addition, the SOA has the following advantages. The SOA is applicableas a modulator by varying the injection current in response to amodulation signal. The SOA can be integrated with an electro absorptionmodulator (EA modulator) and the like.

Next, typical configuration examples of the optical modulation apparatususing the SOAs will be described.

CONVENTIONAL EXAMPLE 1

FIG. 3 shows as a conventional example 1 a configuration of aconventional optical modulation apparatus applicable to the opticalintensity modulator 105 as shown in FIG. 1. The system of theconventional example 1 is drawn assuming that an SOA is used as amodulator 306, and an optical modulation apparatus 303 is placed at adistance from a light source. The SOA modulator 306 has its one endcoupled to an input transmission path 301 to which an optical signal isinput and other end coupled to an output transmission path 309 fromwhich the optical signal is output. The input/output transmission paths,however, include optical connectors and splices in addition to a varietyof optical devices such as an optical filter and optical coupler notshown. Furthermore, although omitted from this figure, a wavelengthmulti-demultiplexer is inserted between the input/output transmissionpath 301 and the SOA modulator 306. These components all constitutereflection points. Since the reflection points are present at both endsides of the SOA optical amplifying section 306, the reflection pointsand the SOA constitute an optical cavity, which can make the operationof the SOA unstable. To prevent the defect, optical isolators 305 and307, which allow the light to be transmitted in one direction, areinserted into both sides of the SOA as shown in FIG. 3.

CONVENTIONAL EXAMPLE 2

FIG. 4 shows as a conventional example 2 a configuration of aconventional optical modulation apparatus applicable to the opticalmodulation circuit of FIG. 2. FIG. 4 shows configurations of two typesof optical modulation apparatuses 405 and 407. A first type opticalmodulation apparatus 405 is configured such that a bidirectional opticalamplifier 409 amplifies the optical power of a continuous wavedemultiplexed by a wavelength multi-demultiplexer 403, and an opticalintensity modulator 411 receiving the continuous wave carries outintensity modulation by a data signal to generate modulated lightfollowed to be reflected by an optical reflector 413, and that thereflected light passes through the optical intensity modulator 411 andbidirectional optical amplifier 409 once again. A second type opticalmodulation apparatus 407 is configured such that a bidirectional opticalamplifier 415 amplifies the optical power of the continuous wavedemultiplexed by the wavelength multi-demultiplexer 403, an optical loopconstructed by using an optical circulator 417 receives the continuouswave, and an optical intensity modulator 419 installed in the opticalloop carries out the intensity modulation by the data signal to generatemodulated light, and that the modulated light passes through the opticalcirculator 417 and the bidirectional optical amplifier 415 once again.In the former optical modulation apparatus 405, the optical reflector413 can be a discrete component separated from the optical intensitymodulator 411, or can be affixed to the end face of the opticalintensity modulator 411 as an integrated combination thereof.

As the bidirectional amplifiers 409 and 415 used in the configuration ofFIG. 4, an SOA is suitable because it is enough for these amplifiers toperform single wavelength amplification. Using the SOA as thebidirectional optical amplifiers 409 and 415, however, brings aboutsignal degradation because of the gain scrambling between the continuouswave and modulated light in the saturation region of the gain.Specifically, the continuous wave is modulated by the signal pattern ofthe modulated light within the optical amplifiers 409 and 415.

Therefore it is preferable as illustrated in FIG. 5 that thebidirectional optical amplifiers 409 and 415 be used in an unsaturatedregion in which when the sum of the output powers (or of the inputpowers) of the continuous wave and modulated light from thebidirectional optical amplifiers 409 and 415 is less than certain outputpower (or input power), the gain is kept constant.

(Problems to be Solved)

The configuration of the conventional example 1 as shown in FIG. 3 has aremaining problem of the end face reflection of the SOA device itselfeven if the optical isolators 305 and 307 are inserted into both ends ofthe SOA 306. Generally, the SOA 306 has its end faces applied withantireflection coating to reduce the end face reflectance, and the endface reflectance is usually smaller than the reflectance of thetransmission path reflection. However, when the SQA 306 has a largegain, the cavity effect of the optical modulation apparatus 303increases, thereby making the amplifying operation unstable. In otherwords, the value of the end face reflectance imposes a limit on the gainpermitted for the SOA. Accordingly, to achieve the high gainamplification by the SOA, it is necessary to connect SOAs in cascade asshown in FIG. 6, for example.

As a multi-stage configuration of the SOAS, a two-stage cascadeconfiguration of SOA+EA modulators (which will be described later) isproposed (Relevant Reference 1: Ohman, F.; Bischoff, S.; Tromborg, B.;Mork, J.; “Noise properties and cascadability of SOA-EA regenerators”,Lasers and Electro-Optics Society, 2002. LEOS 2002. The 15th AnnualMeeting of the IEEE, Volume 2, 2002, Pages 895-896). To minimize theeffect of the optical reflection in the multi-stage configuration of theSOAs, although it is possible to insert optical isolators into theinput/output ends of all the multi-stage SOAs as shown in FIG. 6, it isnot desirable from the viewpoint of cost. In addition, the RelevantReference 1 describes nothing about the insertion of the opticalisolators.

As for the configuration of the conventional example 2 as shown in FIG.4, it has reflected light 1 and reflected light 2 at the ends of thebidirectional optical amplifiers (SOA) 409 and 415. Even though the endfaces of bidirectional optical amplifiers 409 and 415 are made to havelow reflectance by the antireflection coating, the reflected light islarge because of the amplification of the power of the reflected lightbefore and after the end face reflection. Thus, the reflected lightinterferes with signal light, and brings about noise. Incidentally, thereflected light 1 and reflected light 2 will be explained later in thedescription of FIG. 8.

DISCLOSURE OF THE INVENTION

The present invention is implemented to solve the foregoing problems.Therefore it is an object of the present invention to provide aneconomical optical modulation apparatus that can reduce the effect ofthe reflected light rays and achieve the stable amplifying function bythe device specification design and device configuration considering theeffect of the reflection passing through the optical amplifiers in theoptical modulation apparatus with a configuration including opticalamplifiers connected in a multi-stage fashion, or in the opticalmodulation apparatus including optical amplifiers as bidirectionaloptical amplifiers.

A first aspect of the present invention implements a stable amplifyingfunction by reducing the effect of reflected light rays from end facesof a bidirectional optical amplifier by imposing a numerical limitationon the relationship between the gain of the bidirectional opticalamplifier and the loss of the optical modulator in a reflection typeoptical modulator including the bidirectional optical amplifier, or in amulti-wavelength collective optical modulation apparatus combining themultiple optical modulators.

A second aspect of the present invention implements a stable amplifyingfunction by reducing the effect of reflected light rays from end facesof a bidirectional optical amplifier by inserting a polarizationrotation means into a reflection type optical modulator including thebidirectional optical amplifier, or into a multi-wavelength collectiveoptical modulation apparatus combining the multiple optical modulators.

A third aspect of the present invention implements both stableamplifying function and cost reduction by reducing the effect ofreflected light rays by interposing optical isolators at every alternateSOAs in a transmission-type optical modulation apparatus includingsemiconductor optical amplifiers (SOAs) connected in a multistagefashion.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram showing a configuration of a conventionaloptical modulation circuit;

FIG. 2 is a block diagram showing a configuration of a conventionalreflection type optical modulation apparatus;

FIG. 3 is a block diagram showing a configuration of a conventionaloptical modulation apparatus utilizing a semiconductor opticalamplifier;

FIG. 4 is a block diagram showing a configuration of a conventionaloptical modulation apparatus utilizing bidirectional optical amplifiers;

FIG. 5 is a graph illustrating an unsaturated region of a semiconductoroptical amplifier;

FIG. 6 is a block diagram showing a configuration conceivable as anoptical modulation apparatus that can achieve high gain amplification bymultistage connection of semiconductor optical amplifiers;

FIG. 7 is a schematic diagram illustrating behavior of reflected lightrays in a multistage connection of a plurality of semiconductor opticalamplifiers;

FIG. 8 is a schematic diagram illustrating reflected light rays of asemiconductor optical amplifier;

FIG. 9 is a schematic diagram illustrating the behavior of reflectedlight rays in a multistage connection of two semiconductor opticalamplifiers;

FIG. 10 is a table illustrating ratios of the reflected light rays tosignal light in FIG. 9;

FIGS. 11A-11C are block diagrams each showing a configuration of anoptical modulation apparatus of a first embodiment in accordance withthe present invention;

FIGS. 12A-12C are block diagrams each showing a configuration of anoptical modulation apparatus of a second embodiment in accordance withthe present invention;

FIG. 13 is a graph illustrating characteristics of an optical modulationapparatus of a third embodiment in accordance with the presentinvention;

FIG. 14 is a block diagram showing a configuration of an opticalmodulation apparatus of a fourth bodiment in accordance with the presentinvention;

FIG. 15 is a schematic diagram illustrating directions of planes ofpolarization in the fourth embodiment in accordance with the presentinvention; and

FIG. 16 is a block diagram showing a configuration of an opticalmodulation apparatus of a fifth embodiment in accordance with thepresent invention.

BEST MODE FOR CARRYING OUT THE INVENTION

The best mode for carrying out the invention will now be described withreference to the accompanying drawings.

First Embodiment

The first embodiment in accordance with the present invention has, in atransmission-type optical modulation apparatus including semiconductoroptical amplifiers (SOAs) connected in cascade, optical isolatorsinserted at every alternate units to reduce the effect of the reflectedlight, thereby implementing the stable amplifying function and costreduction at the same time. Before describing concrete configurationexamples of the present t, its principle will be explained.

<Reflected Light in Multistage Connection of SOAS>

FIG. 7 is a diagram illustrating reflected light rays when a pluralityof SOAs are arranged in the multistage connection. In the multistageconnection, to operate it as an optical modulation apparatus, one of theSOAs must be used as an optical intensity modulator, or an externalmodulator must be inserted. However, to simplify the description of thereflected light rays here, the SOAs are assumed to function just as anoptical amplifier.

In FIG. 7, n (>=2) semiconductor optical amplifiers (S₁, S₂, . . . ,S_(i), . . . , S_(n)) are coupled in series via n+1 optical paths (x₁,x₂, . . . , x_(i), . . . , x_(n+1)) inclusive of input/output pathswhich are connected to an input-side transmission path 301 and anoutput-side transmission path 309, respectively. As described above, theinput/output transmission paths 301 and 309 constitute a reflectionpoint. In addition, since the SOAs (S₁, S₂, . . . , S_(i), . . . ,S_(n)) have reflection ends at both ends of the devices themselves, theSOAs become reflection points by themselves.

FIG. 8 is a diagram illustrating the reflected light rays of the SOA.Assume that the SOA has a gain g_(i), and end face reflectance r, then,when light with optical power 1 is input to the SOA, the SOA hasreflection optical power of g_(i) ²r. This means that the end facereflectance is multiplied by g_(i) ². The reflection can take placebidirectionally in every SOA.

In FIG. 7, the reflections in the traveling direction of the signallight are designated by Ref(0), Ref(1), . . . , Ref(i), and Ref(n) inthis order from the input side, and the reflections in the oppositedirection of the signal light are designated by ref (1), ref (2), . . ., ref(i), and ref(n+1) in this order from the input-side. The Ref(0) andref(n+1) are input-side transmission path reflection and output-sidetransmission path reflection, respectively, and the remainingreflections Ref(i) and ref(i) represent bidirectional reflections of thesemiconductor optical amplifier S_(i).

The effect of the reflected light rays will be considered in the case ofn=2 for simplicity. FIG. 9 is a diagram illustrating the reflected lightrays when n=2. The symbols Ref(0), Ref(1) and Ref(2) designate thereflections in the traveling direction of the signal light, and thesymbols ref(1), ref(2) and ref(3) designate the reflections in theopposite direction. The Ref(0) and ref(3) designate the input-sidetransmission path reflection and output-side transmission pathreflection, respectively, and Ref (1) and ref (1), and Ref (2) and ref(2) are the reflections of the semiconductor optical amplifiers S₁ andS₂, respectively. The reflection becomes a problem because following thereflection (first reflection) in the direction opposite to the travelingdirection of the signal light, the reflection (second reflection) in thetraveling direction occurs, which will make the signal optical powerunstable because of interference with the signal light. In FIG. 9, sincethe SOAs have a gain, the reflected light rays are amplified by thatgain, which enhances the effect.

FIG. 10 is a table illustrating ratios of the twice reflected light raysto the signal light when the reflectances of the Ref(i) and ref(i) inFIG. 9 are assumed to be R(i) and r(i) (where 1<=i <=3). As shown inFIG. 10, when Ref(i−1) reflection occurs following ref(i), the ratios ofthe twice reflected light rays to the signal light are in the order of asquare of the reflectance at the reflection point. However, when thereflection Ref(i−2) or Ref(i−3) occurs following ref(i), the ratio ofthe twice reflected light rays to the signal light is increased by asquare of the gain of the SOA passed through as compared with the orderof the square of the reflectance at the reflection point. Although FIG.10 shows the case where n=2, when n SOAs are arranged in the multistageconnection, the reflections Ref(i−2), Ref(i−3), . . . , and Ref(0)following ref(i) have the ratios of the reflected light rays to thesignal light greater than the reflection Ref(i−1) following ref(i) bysquares of the gains of S_(i−1), S_(i−1)+S_(i−2), . . . , S_(i−1),S_(i−2)+ . . . S₁ (where 1<=i<=n+1).

Accordingly, to allow the reflection Ref(i−1) following ref(i), and toprevent reflections Ref(i−2), Ref(i−3), . . . , and Ref(0) following ref(i), it is enough to insert optical isolators at every alternate opticalpath (x₁, x₂, . . . , x_(i), . . . , x_(n+1)).

CONCRETE CONFIGURATION EXAMPLE

FIGS. 11A-11C are diagrams illustrating configurations of the opticalmodulation apparatus of the first embodiment in accordance with thepresent invention, into which optical isolators are inserted at everyalternate optical path. Here, O₁ and O₂ each designate an opticalisolator. The first optical isolator O₁ is inserted into the firstoptical path x₁ between the input-side transmission path and the firstSOA S₁, and the second optical isolators O₁ is inserted into the thirdoptical path x₃ between the second SOA S₂ and third SOA S₃. Thus, thepresent embodiment is characterized by inserting the optical isolatorsat every alternate optical path.

In addition, the present examples each include n=3 SOAs, and use any oneof them as an optical intensity modulator (MOD) by carrying outintensity modulation of injection current by a transmission signal.Specifically, the third SOA S₃ is used as the optical intensitymodulator in FIG. 1A, the second SOA S₂ is used as the optical intensitymodulator in FIG. 11B, and the first SOA S₁ is used as the opticalintensity modulator in FIG. 1C.

As for the foregoing relationship of the arrangement of the opticalisolators and the optical intensity modulator, it is the same when thenumber of the SOAs is two or four or more.

The configuration of the embodiment can implement the system that cancompensate for the optical power loss on the transmission path andachieve the modulation operation simultaneously in the opticalcommunication system having the light source for outputting thecontinuous wave and the optical intensity modulator, which are placed ata distance via the transmission path.

Second Embodiment

FIGS. 12A-12C are diagrams each showing a configuration of the opticalmodulation apparatus of a second embodiment in accordance with thepresent invention. The present embodiment is a variation of the firstembodiment, which has an optical intensity modulator M inserted betweenany two of three SOAs S₁, S₂ and S₃ constituting the optical amplifier.

FIG. 12A shows a configuration having the optical intensity modulator Minserted into a section in which neither the optical isolator O₁ nor O₂is inserted. Although the example is shown here which has the opticalintensity modulator M inserted into the second optical path (opticalconnection means) x₂ between the first and second SQAs S₁ and S₂, theoptical intensity modulator M can be inserted into a fourth optical path4 between the third SOA S₃ and the output terminal. In the latter case,however, it is necessary to use an optical intensity modulator M thatcan handle the optical power amplified by the final stage SOA S₃.

In the configuration of FIG. 12A, the intensity modulation is carriedout twice by the optical intensity modulator M until the continuous waveoutput from the first SOA S₁ interferes with the twice reflected lightray of the continuous wave at the second SOA S₂ and first SOA S₁.Accordingly, the ratio of the twice reflected light ray to the signallight is relatively small as comprised with the case where no opticalintensity modulator M is inserted.

FIG. 12B shows a configuration that has the optical intensity modulatorM inserted into the section into which the optical isolator O₂ isinserted. Although the example shown has the optical intensity modulatorM inserted into the third optical path x₃ between the second and thirdSOA S₂ and S₃, the optical intensity modulator M can be inserted intothe first optical path x₁ between the input terminal and the first SOAS₁. In the latter case, however, it is necessary to consider that theinput power to the SOA S₁ is reduced and the SNR is deteriorated becauseof the loss of the optical intensity modulator M. Incidentally, theorder of connection of the optical isolator O₂ and the optical intensitymodulator M is arbitrary as shown in FIGS. 12B-12C.

As the optical intensity modulator M used in the present embodiment, anelectro absorption optical intensity modulator (EA modulator) can beused, for example. Since the foregoing first embodiment uses the SOA asthe optical intensity modulator, it is difficult to carry out themodulation operation of the order of G (bps) or more. In contrast, theEA modulator used as the optical intensity modulator can handle themodulation operation of the order of 40G (bps).

Third Embodiment

A third embodiment of the optical modulation apparatus in accordancewith the present invention relates to a system that can achieve thestable amplifying function by reducing the effect of the reflected lightrays on the end faces of the bidirectional optical amplifiers byimposing the following numerical limitation on the gain of the amplifierin the foregoing system configuration including the bidirectionaloptical amplifiers as shown in FIG. 4. The numerical limitation on theamplifier gain in accordance with the present invention will bedescribed below.

<Method of Quantifying Effect of Reflected Light>

As shown in FIG. 4, there are two reflected light rays from the ends ofthe bidirectional optical amplifier 409 or 415: first reflected light 1travels in the same direction as the modulated light, and secondreflected light 2 travels in the same direction as the continuous wave.The continuous wave undergoes the intensity modulation and becomes themodulated light. Since the reflected light 2 travels through the samepath as the continuous wave, the modulated light is finally providedwith the reflected light 1 and reflected light 2. The modulated lightinterferes with the same polarization direction components of thereflected light 1 and reflected light 2, thereby generating intensityfluctuations as beat noise. Next, a method will be described ofquantitatively showing the effect of the reflected light 1 and reflectedlight 2 on the modulated light.

The following are assumed here.

-   -   The multiple reflection light rays, which are reflected off the        first end face of the bidirectional optical amplifier 409 or 415        and then reflected off the second end face thereof again, are        assumed to be sufficiently small and are neglected.    -   The mark-to-space ratio of the transmission signal is assumed to        be 1/2. (Since the continuous mark or space in the data signal        train makes it difficult to extract a clock signal at the        reception of the signal, a technique of making the mark-to-space        ratio nearly 1/2 is usually employed such as scramble in the SDH        (synchronous digital hierarchy) or 8 B→10 B (bel) conversion in        the gigabit ether.)

Assume that the input continuous wave power to the bidirectional opticalamplifiers 409 and 415, the gain of the bidirectional optical amplifiers409 and 415, the difference between the modulated light output power andthe input continuous wave power to the optical intensity modulators 411and 419, and the reflectance of the entire bidirectional opticalamplifier are l, g, x and r′, respectively, then the modulation opticalpower of the optical modulator output, the power of the reflected light1, and the power of the reflected light 2 are represented by g₂x, r′ andg²x²r′, respectively.

Since the problem to be considered here is the interference between themodulated light and the reflected light, it is enough to consider onlythe effect of the reflected light when the modulated light is at themark. Since the transmission signal has the mark-to-space ratio of 1/2,the mark level power of the output modulated light of the opticalmodulator, and the mark level power of the reflected light 2 are 2gx and4g²x²r′, respectively. Here, since the probability is 1/2 that themodulated light and reflected light 2 are mark at the same time in theoptical modulator output, the effect of the reflected light 2 is halved.Accordingly, the power ratio between the modulated light and the totalreflected light when the modulated light is at the mark is expressed by$\begin{matrix}{\frac{S}{N} = \frac{2g^{2}x}{\left( {r^{\prime} + {2g^{2}x^{2}r^{\prime}}} \right)}} & (1)\end{matrix}$In addition, since r′ has a relationship of r′=g²r when the fibercoupling loss is neglected, it can be rewritten as $\begin{matrix}{\frac{S}{N} = \frac{2g^{2}x}{\left( {{g^{2}r} + {2g^{4}x^{2}r}} \right)}} & (2)\end{matrix}$Considering expression (2) as a function of x, expression (2) takes amaximum value when $\begin{matrix}{x = \frac{1}{\sqrt{2}g}} & (3)\end{matrix}$In other words, the effect of the reflected light rays can be minimizedat that value. Rewriting it using a logarithmic scale and thetransmission path loss L[dB] and bidirectional amplifier gain G[dB], thefollowing expression holds. $\begin{matrix}{L = {{{- 10}{\log_{10}(x)}} = {{{10{\log_{10}(g)}} + {{\frac{1}{2} \cdot 10}{\log_{10}(2)}}} = {G + 1.5}}}} & (4)\end{matrix}$In this case, the power of the reflected light 1 becomes equal to thatof the reflected light 2.

In actuality, since the reflected light interferes with the modulatedlight, the foregoing description is effective only for derivingexpression (4) above that optimizes the SNR. The quantitative estimationof the effect of the reflected light on the modulated light can be madeas follows.

Consider the case where the optical modulator output is received throughthe optical circulator 417 or the like. Assume that mark-side opticalelectrical field of the modulated light is E₀ exp[i(ω_(c)t+φ₀)],mark-side optical electrical field of the reflected light 1 is E₁exp[i(ω_(c)t+φ₁)], and mark-side optical electrical field of thereflected light 2 is E₂ exp[i(ω_(c)t+ω₂)], then the optical electricalfield before reception is expressed by the following expression.E _(OUT)(t)=E ₀ exp[i(ω_(c) t+φ ₀)]+E ₁ exp[i(ω_(c) t+φ ₁)]+E ₂exp[i(ω_(c) t+φ ₂)]  (5)

The received optical current is given by the following expression byneglecting all the coefficients required. $\begin{matrix}{i_{p} = {E_{0}^{2} + {2E_{0}E_{1}{\exp\left\lbrack {i\left( {\phi_{0} - \phi_{1}} \right)} \right\rbrack}} + {2E_{0}E_{2}{\exp\left\lbrack {i\left( {\phi_{0} - \phi_{2}} \right)} \right\rbrack}} + E_{1}^{2} + E_{2}^{2} + {2E_{1}E_{2}{\exp\left\lbrack {i\left( {\phi_{1} - \phi_{2}} \right)} \right\rbrack}}}} & (6)\end{matrix}$Here, the first term is the modulated light itself, and the second andsubsequent terms are noise. The first term to sixth term represent whenthe modulated light and reflected light are all on the mark-side: themodulation optical power; the beat (interference) between the modulatedlight and the reflected light 1; the beat (interference) between themodulated light and the reflected light 2; the power of the reflectedlight 1; the power of the reflected light 2; and the beat (interference)between the reflected light 1 and the reflected light 2. The fourth tosixth terms are negligible because the reflected light is small ascompared with the modulated light. Here, considering the second andthird terms, normalized beat noise power is defined as follows.$\begin{matrix}{\sigma_{RIN}^{2} = \frac{2\left( {{E_{0}^{2}E_{1}^{2}} + {E_{0}^{2}E_{2}^{2}}} \right)}{\left( E_{0}^{2} \right)^{2}}} & (7)\end{matrix}$

The beat noise when a plurality of reflection points are involved can behandled as Gaussian distribution with a variance given by expression(7). On the contrary, when the number of the reflection points is small,excessive estimation of the beat noise is made.

The above discussion so far considers as the reflected light rays thereflected light 1 and reflected light 2 from both end faces of thebidirectional optical amplifiers 409 and 415. In practice, however,besides the end face reflections at the bidirectional optical amplifiers409 and 415, there are input/output terminal reflections of a variety ofoptical devices inserted into the system, and reflections by opticalconnectors, and the reflected light rays from these reflection pointsundergo the gains of the bidirectional optical amplifiers 409 and 415,and become nonnegligible depending on their reflectances. In such acase, considering the end face reflectance r used in the discussion upto now as the sum of the reflectances of the reflection points otherthan the end face reflection, it can be correctly said that theestimation of the effect of the reflected light rays using the variancegiven by expression (7) is appropriate. On the other hand, when thereflections from both end faces of the bidirectional optical amplifiers409 and 415 are dominant, it is appropriate to consider the foregoingestimation as the worst case.

The foregoing discussion is made on the analogy of the paper IEEE J.Lightwave Tchnol., vol. 14, no. 6, pp. 1097-1105, 1996 describing amethod of quantitatively estimating the effect of the coherent crosstalkof an arrayed-waveguide grating (AWG). However, in the present opticalmodulation apparatus, since the probability that the reflected light 2is mark when the modulated light is mark is 1/2, the foregoingexpression (7) can be rewritten by the following expression.$\begin{matrix}{\sigma_{RIN}^{2} = \frac{{2E_{0}^{2}E_{1}^{2}} + {E_{0}^{2}E_{2}^{2}}}{\left( E_{0}^{2} \right)^{2}}} & (8)\end{matrix}$The value of the expression is equal to twice the reciprocal of theforegoing expression (2).<Calculation Example of Effect of Reflected Light>

FIG. 13 shows calculation results using the foregoing expression (8). InFIG. 13, the horizontal axis represents a modulation section loss (L)[dB], and the vertical axis represents a Q value [dB] on the left side,and the optical modulation apparatus gain [dB] on the right side. As forthe optical modulation apparatus gain, are drawn both 2G−(L−3.0) [dB]without considering the 3 dB modulation loss in the modulation section(optical intensity modulators) 411 or 419, and 2G−L [dB] considering the3 dB modulation loss. The Q value here refers to an evaluation parameterthat determines the signal-to-noise ratio (SNR) of the modulated lightproposed in IEEE Photon. Technol. Lett. Vol. 5, no. 3, pp. 304-306, andis defined by the following expression $\begin{matrix}{Q = \frac{{S(1)} - {S(0)}}{\sigma_{1} + \sigma_{0}}} & (9)\end{matrix}$where S(1) and S(0) indicate the signal levels of the mark and space,respectively, and σ₁ and σ₀ represent noise quantities of mark andspace, respectively. Here, assume that S(1)=1, then σ₁=σ_(RN), and S(0)and σ₀ are considered nearly zero.

It is assumed in the calculation that the input continuous wave power tothe optical modulation apparatuses 405 and 407 is −6 dBm, thebidirectional optical amplifier gain G is 10 [dB], the bidirectionaloptical amplifier noise factor is 7 dB, and the total reflectance of thebidirectional optical amplifier is −22 dB, and that the modulated lightis received by direct photoelectric conversion rather than by opticalpreamplifier reception. As shown in FIG. 13, which illustrates thecalculation results, the Q value takes a maximum value when themodulation section loss L=11.5 [dB], that is, when L=G+1.5 [dB], and thecurve representing the Q value has left-right symmetry with respect tothe center having that value. In FIG. 13, ranges (a), (i), (γ) and (δ)are as follows.

(α) 0<=L<=2G+3.0

The optical modulation section loss region that ensures the opticalmodulator gain 2G−(L−3.0)>=0, and the Q value with the optical modulatorgain 2G−(L−3.0)=0 (dB).

(β) 3.0<=L<=2G

The optical modulation section loss region that ensures the opticalmodulator gain 2G−L>=0, and the Q value with the optical modulator gain2G−L=0 (dB).

(γ) G−4.5<=L<=G+7.5

The region where the Q value is within 3 dB of the maximum value.

(δ) L=G+1.5

The modulation section loss that takes the maximum Q value.

As for the region (δ), it is as described above. In addition, the upperlimit values of L in the regions (α) and (β) indicate that the opticalmodulation gain is equal to or greater than 0 [dB]. Furthermore, as forthe modulation section loss L, its value is logically determined fromthe fact that the Q value curve has the left-right symmetry as describedabove.

The Q value becomes within 3 dB with respect to the maximum value when5.5 [dB]<=L<=17.5 [dB], that is, (G+1.5)-6 [dB]<=L<=(G+1.5)+6 [dB]. Therange of L is independent of the value G. In fact, solving the quadraticequation for x, which is obtained by substituting the value x defined inthe foregoing expression (3) into the foregoing expression (1), and bymaking the half of that result (3 dB reduction) equal to expression (1),gives the following solution. $\begin{matrix}{x = \frac{\left( {{2\sqrt{2}} \pm \sqrt{6}} \right)}{2g}} & (10)\end{matrix}$In addition, rewriting it in the logarithmic scale gives the following.$\begin{matrix}\begin{matrix}{L = {{- 10}{\log_{10}(x)}}} \\{= {{10{\log_{10}\left( \frac{2}{{2\sqrt{2}} \pm \sqrt{6}} \right)}} + {10{\log_{10}(g)}}}} \\{\cong {\left( {G + 1.5} \right) \pm 6}}\end{matrix} & (11)\end{matrix}$It indicates the upper limit value and lower limit value of the region(γ).

Accordingly, with maintaining the gain, the optical modulation apparatuscan keep the ratio low of the reflected light to the modulated lightwith placing the modulation section loss L in a given range in theregion (α) (such as (β), (γ) and (δ)). In this case, as is clear fromFIG. 13, the ratio can be reduced as the modulation section loss Lapproaches L=G+1.5 at (δ).

Fourth Embodiment

FIG. 14 shows a configuration of the optical modulation apparatus of afourth embodiment in accordance with the present invention. The opticalmodulation apparatus of the present embodiment implements a stableamplifying function by reducing the effect of the reflected light fromthe end faces of the bidirectional optical amplifiers by insertingpolarization rotation means.

As shown in FIG. 14, the present system is a multi-wavelength collectiveoptical modulation apparatus that includes a polarization demultiplexer501 for separating the input multi-wavelength light from the outputmodulated light by the difference in the plane of polarization; awavelength multi-demultiplexer 502 for demultiplexing themulti-wavelength light into every predetermined wavelengths;bidirectional optical amplifiers 503 for bidirectionally amplifying theindividual single wavelength optical powers demultiplexed; polarizationrotation means 504 each for bidirectionally rotating the plane ofpolarization of the single wavelength light; optical intensitymodulators 505 each for bidirectionally modulating the intensity of thesingle wavelength light; and optical reflectors 506 for feeding themodulated single wavelength light rays output from the optical intensitymodulators 505 back to the bidirectional optical amplifiers 503.

As the polarization demultiplexer 501, a polarization beam splitter(PBS) is applicable. Alternatively, a configuration is also possiblewhich has the wavelength multi-demultiplexer 502 produce output lightvia an optical circulator or an optical coupler, and extracts the lightwhose polarization shifts from that of the input light by 90 degrees byusing a polarizer.

As the wavelength multi-demultiplexer 502, an AWG is applicable, forexample. The AWG has the light incident onto an input waveguide outputfrom a different output waveguide in accordance with the wavelength. TheAWG has reversibility, and can multiplex a plurality of wavelength lightrays into a single output waveguide.

As the bidirectional optical amplifiers 503, SOAs can be used, forexample. The SOA is an optical amplifier for amplifying the lighttraveling through the active layer in the semiconductor by stimulatedemission by reducing the reflection from the cavity end faces of asemiconductor laser. As the bidirectional optical amplifiers 503, fiberamplifiers such as erbium doped fiber amplifiers (EDFAs) can also beused. However, since the fiber amplifier is composed of a semiconductorlaser for outputting pumping light, a doped fiber doped with erbium andthe like, and a coupler for coupling the pumping light to the dopedfiber, it will be more expensive than the SOA from the viewpoint of thenumber of the components. Accordingly, the SOA has a cost advantage.

The polarization rotation means 504 is installed between thebidirectional optical amplifiers 503 and the optical intensitymodulators 505. As the polarization rotation means 504, a quarter-waveplate or a Faraday cell is applicable. Alternatively, a Faraday mirroris usable which attaches a reflecting mirror to an output end of theFaraday cell.

As the optical intensity modulators 505, a Mach Zehnder type opticalintensity modulator or an electro absorption optical intensity modulator(EA modulator) is applicable, for example. They have a function ofcarrying out intensity modulation of the single wavelength light by adata signal. These optical intensity modulators can achieve theintensity modulation by a 40 G(bps) order modulation signal at apractical level.

As the optical reflectors 507, a mirror having metal coating ordielectric multi-layer coating is applicable, for example. As areflecting mirror for a particular wavelength, a diffraction grating orfiber Bragg grating is also applicable to the optical reflector. Inaddition, as an application of the fiber Bragg grating, an opticalreflector can be used in which a diffraction grating is directly writtenon an optical waveguide.

One of the output ports of the polarization demultiplexer 501 isoptically connected to the input waveguide of the wavelengthmulti-demultiplexer 502 via a spatial optical system or an opticalwaveguide. The output waveguides of the wavelength multi-demultiplexer502 are optically connected to first ports of the bidirectional opticalamplifiers 503 via a spatial optical system or optical waveguides.Second ports of the bidirectional optical amplifiers 503 are opticallyconnected to first ports of the polarization rotation means 504 via aspatial optical system or optical waveguides as well. Second ports ofthe polarization rotation means 504 are optically connected to firstports of the optical intensity modulators 505 via a spatial opticalsystem or optical waveguides as well. Second ports of the opticalintensity modulators 505 are optically connected to the opticalreflectors 507 via a spatial optical system or optical waveguides aswell.

In the present embodiment, the polarization demultiplexer 501 separatesthe inputs to the optical intensity modulators 505 from their modulatedlight outputs. However, in the case where the quarter-wave plates areused as the polarization rotation means 504, the angles of the planes ofpolarization of the input light rays and the output light rays differ by90 degrees. Accordingly, the input light rays can be separated from theoutput light rays by extracting the particular polarized waves from theoutput light rays by the polarization demultiplexer 501.

The multi-wavelength light input to the wavelength multi-demultiplexer502 via the input waveguide is demultiplexed to the individualwavelengths by the wavelength multi-demultiplexer 502. Each singlewavelength light passing through the demultiplexing is led tocorresponding one of the bidirectional optical amplifiers 503 to haveits power amplified.

The bidirectional optical amplifiers 503 bring about signal degradationbecause of the gain scrarbling between the continuous waves andmodulated light rays in the saturation region of the gain. Accordingly,as illustrated in FIG. 5, it is preferable that the bidirectionaloptical amplifiers 503 be used in the unsaturated region of the gain inwhich the gain (the vertical axis) is maintained at a constant value aslong as the sum of the output powers (the horizontal axis) (or the sumof input powers) of the continuous waves and the modulated light fromthe bidirectional optical amplifiers 503 is equal to or less than aparticular output power (or input power).

The continuous waves (single wavelength light rays) whose powers areamplified by the individual bidirectional optical amplifiers 503 areinput to the corresponding polarization rotation means 504. Thepolarization rotation means 504 rotate the planes of polarization of thecontinuous waves by 45 degrees, and supply them to the optical intensitymodulators 505. The optical intensity modulators 505 carry out theintensity modulation of the continuous waves by modulation signals (datasignals). The modulated single wavelength light rays are output from theoptical reflectors side ports of the optical intensity modulators 505,and are input to the optical reflectors 507. The modulated light raysreflected by the optical reflectors 507 pass through the opticalintensity modulators 505 again, and are input to the polarizationrotation means 504. The modulated light rays have their planes ofpolarization rotated by 45 degrees by the polarization rotation means504, and are input to the bidirectional optical amplifiers 503 whichamplify the optical powers again. Since the output modulated light raysof the bidirectional optical amplifiers 503 have the planes ofpolarization different by 90 degrees from those of the input light rays,the polarization denultiplexer 501 can separate the output light raysfrom the input light rays. Accordingly, the output modulated light raysfrom the bidirectional optical amplifiers 503 are multiplexed by thewavelength multi-demultiplexer 502, and are output from the output portof the polarization denultiplexer 501 to a system outside.

To operate the optical amplifier in the bidirectional mode, the opticalamplifier cannot include an optical isolator. Accordingly, it isnecessary to consider the effect of the end face reflections from bothterminals of the optical amplifying paths. As shown in FIG. 4, there aretwo reflected light rays in the bidirectional transmission (reflectedlight ray 1 and reflected light ray 2). The reflected light ray 1propagates in the same direction as the modulated light, and thereflected light ray 2 in the same direction as the continuous waves. Thecontinuous waves undergo the intensity modulation and become modulatedlight, and the reflected light ray 2 travels through the same path asthe continuous waves. Consequently, if the planes of polarization of thereflected light rays 1 and 2, continuous waves, and modulated light raysare the same as in the conventional example, the modulated light raysare provided with the reflected light ray 1 and reflected light ray 2.As a result, the modulated light rays interfere with the samepolarization direction components of the reflected light ray 1 andreflected light ray 2, causing the intensity fluctuations as the beatnoise.

However, in the configuration of the present embodiment having thepolarization rotation means 504, the reflected light ray 1 and reflectedlight ray 2 from the bidirectional optical amplifiers 503 are orthogonalto the polarization direction of the continuous waves or modulated lightrays traveling in the same direction as indicated by arrows enclosed bycircles representing the directions of the planes of polarization inFIG. 15. Since the reflected light ray 1 and the modulated light rayshave the polarization directions orthogonal to each other, thepolarization demultiplexer 501 can separate them at the output. Inaddition, the reflected light ray 2 has the polarization directionorthogonal to that of the continuous waves, and maintain thepolarization relationship after the reflected light ray 2 passes throughthe intensity modulation and become modulated light rays. Thus, thereflected light ray 2 can be separated from the continuous waves so asto output by the polarization demultiplexer 501 in the same manner asthe reflected light ray 1. As a result, the intensity fluctuations dueto the interference between the two light rays can be eliminated.

According to the configuration of the present ement, as shown in FIG.15, the planes of polarization of the light rays are the same in the twodirections on the paths from the outputs of the polarization rotationmeans 504 to the return to the polarization rotation means 504 after thereflection by the optical reflectors 507. Consequently, it is possibleto use as the optical intensity modulators 505 an optical intensitymodulator such as LiNbO₃ Mach Zehnder type optical intensity modulatorcapable of carrying out modulation only for a single input polarizedwave.

Fifth Embodiment

FIG. 16 shows a configuration of the optical modulation apparatus of afifth embodiment in accordance with the present invention. The system ofthe fifth embodiment has polarizers 506, which enable only singlepolarized waves to pass through, interposed before or after the opticalintensity modulators 505 of the multi-wavelength collective opticalmodulation apparatus in the foregoing fourth embodiment (in FIG. 16,they are interposed after). Since the remaining configuration is thesame as that of the fourth embodiment, the detailed description thereofis omitted here.

Generally speaking, the polarization extinction ratio between twoorthogonal polarized waves deteriorates markedly when coupling aplurality of optical devices and fibers. According to the configurationshown in FIG. 16, since the planes of polarization of the light rays arethe same in the two directions on the paths from the outputs of thepolarization rotation means 504 to the return to the polarizationrotation means 504 after the reflection by the optical reflectors 507,the polarizers 506 can be inserted into the optical paths. The insertionof the polarizers 506 can recover the polarization extinction ratiodegraded.

Other Embodiments

The present invention has been described by way of example of preferredembodiments. However, the embodiments in accordance with the presentinvention are not limited to the foregoing examples, and a varietymodifications such as replacement, changes, addition, increase ordecrease in the number, or the changes in the geometry of the componentsof the configuration are all included in the embodiments in accordancewith the present invention as long as they fall within the scope of theclaims.

1. An optical modulation apparatus comprising: bidirectional opticalamplifying means for transmitting a continuous wave with a singlewavelength bidirectionally, and for providing the single wavelengthlight with a gain; optical intensity modulation means for carrying outintensity modulation of the continuous wave whose optical power isamplified by said bidirectional optical amplifying means, by atransmission signal with a mark-to-space ratio of practically 1/2; andoptical regression means for feeding the continuous wave passing throughthe intensity modulation by said optical intensity modulation means backto said optical intensity modulation means, or back to saidbidirectional optical amplifying means directly, wherein a modulationsection loss L (dB), which is defined as a difference between opticalpower of the input continuous wave to said optical intensity modulationmeans and optical power of output modulated light from said opticalintensity modulation means to a gain G (dB) of said bidirectionaloptical amplifying means, is set in a range from 0 (dB) to 2G+3.0 (dB).2. The optical modulation apparatus as claimed in claim 1, wherein themodulation section loss L (dB) is set at G+1.5 (dB).
 3. The opticalmodulation apparatus as claimed in claim 1, wherein said bidirectionaloptical amplifying means is operated in an unsaturated region of thegain.
 4. The optical modulation apparatus as claimed in claim 2, whereinsaid bidirectional optical amplifying means is operated in anunsaturated region of the gain.
 5. The optical modulation apparatus asclaimed in claim 1, wherein said optical intensity modulation means is areflection type optical intensity modulator having an optical reflectorconstituting said optical regression means at a rear end of said opticalintensity modulation means.
 6. The optical modulation apparatus asclaimed in claim 1, wherein said optical intensity modulation means is atransmission-type optical intensity modulator that is installed in anoptical loop constituting said optical regression means formed via anoptical circulator.
 7. The optical modulation apparatus as claimed inclaim 1, wherein said optical modulation apparatuses equal in number tomultiplexed wavelengths are installed, and further comprise wavelengthmulti-demultiplexing means for demultiplexing continuous waves which arewavelength division multiplexed, for supplying each single wavelength toone of a plurality of said optical modulation apparatus, and formultiplexing modulated light rays output from said plurality of opticalmodulation apparatuses to be output.
 8. An optical modulation apparatuscomprising: a plurality of sets each of which includes: bidirectionaloptical amplifying means for transmitting single wavelength lightbidirectionally which constitutes multi-wavelength light including aplurality of optical carriers, and for providing the single wavelengthlight with a gain; optical intensity modulation means for modulating thesingle wavelength light by transmitting the single wavelength lightbidirectionally which is provided with the gain by said bidirectionaloptical amplifying means; and optical regression means for regressingthe single wavelength light transmitting through said optical intensitymodulation means to said optical intensity modulation means again,wherein said plurality of sets are provided in correspondence to theplurality of single wavelength light rays constituting themulti-wavelength light; wavelength multi-demultiplexing means fordemultiplexing the multi-wavelength light into single wavelength lightrays, for inputting the single wavelength light rays into saidbidirectional optical amplifying means, and for multiplexing a pluralityof single wavelength light rays output from said bidirectional opticalamplifying means again; a plurality of polarization rotation means eachinterposed between said bidirectional optical amplifying means and saidoptical intensity modulation means, for rotating a plane of polarizationof each one of the single wavelength light rays; and polarizationdemultiplexing means for supplying input multi-wavelength light to saidwavelength multi-demultiplexing means, for separating from the inputmulti-wavelength light, output multi-wavelength light which has itsplane of polarization rotated by said polarization rotation means and isoutput from said wavelength multi-demultiplexing means, and foroutputting the demultiplexed output multi-wavelength light.
 9. Theoptical modulation apparatus as claimed in claim 8, further comprisingpolarizers interposed before or after said optical intensity modulationmeans.
 10. An optical modulation apparatus comprising: n semiconductoroptical amplifiers for generating population inversion by individualinjection currents, where n satisfies n>=2; (n+1) optical connectionmeans for successively connecting an input terminal, said nsemiconductor optical amplifiers and an output terminal; opticalisolators successively interposed at even number or odd number positionsof said (n+1) optical connection means; and optical intensity modulationmeans for carrying out intensity modulation of a continuous wave. 11.The optical modulation apparatus as claimed in claim 10, wherein one ofsaid n semiconductor optical amplifiers is supplied with the injectioncurrent undergoing intensity modulation by a transmission signal, and ismade said optical intensity modulation means.
 12. The optical modulationapparatus as claimed in claim 10, wherein said optical intensitymodulation means is interposed into one of said (n+1) optical connectionmeans.
 13. The optical modulation apparatus as claimed in claim 10,wherein said optical intensity modulation means is interposed into oneof said (n+1) optical connection means except for the optical connectionmeans connected to said input terminal and said output terminal.
 14. Theoptical modulation apparatus as claimed in claim 12, wherein saidoptical intensity modulation means is interposed into optical connectionmeans of said (n+1) optical connection means, which have none of saidoptical isolators interposed.
 15. The optical modulation apparatus asclaimed in claim 13, wherein said optical intensity modulation means isinterposed into optical connection means of said (n+1) opticalconnection means, which have none of said optical isolators interposed.16. The optical modulation apparatus as claimed in claim 2, wherein saidoptical intensity modulation means is a reflection type opticalintensity modulator having an optical reflector constituting saidoptical regression means at a rear end of said optical intensitymodulation means.
 17. The optical modulation apparatus as claimed inclaim 3, wherein said optical intensity modulation means is a reflectiontype optical intensity modulator having an optical reflectorconstituting said optical regression means at a rear end of said opticalintensity modulation means.
 18. The optical modulation apparatus asclaimed in claim 2, wherein said optical intensity modulation means is atransmission-type optical intensity modulator that is installed in anoptical loop constituting said optical regression means formed via anoptical circulator.
 19. The optical modulation apparatus as claimed inclaim 3, wherein said optical intensity modulation means is atransmission-type optical intensity modulator that is installed in anoptical loop constituting said optical regression means formed via anoptical circulator.
 20. The optical modulation apparatus as claimed inclaim 2, wherein said optical modulation apparatuses equal in number tomultiplexed wavelengths are installed, and further comprise wavelengthmulti-demultiplexing means for demultiplexing continuous waves which arewavelength division multiplexed, for supplying each single wavelength toone of a plurality of said optical modulation apparatus, and formultiplexing modulated light rays output from said plurality of opticalmodulation apparatuses to be output.